Leakage in Nanometer CMOS TechnologiesSiva G. Narendra, Anantha P. Chandrakasan Springer Science & Business Media, 2006. gada 10. marts - 308 lappuses Scaling transistors into the nanometer regime has resulted in a dramatic increase in MOS leakage (i.e., off-state) current. Threshold voltages of transistors have scaled to maintain performance at reduced power supply voltages. Leakage current has become a major portion of the total power consumption, and in many scaled technologies leakage contributes 30-50% of the overall power consumption under nominal operating conditions. Leakage is important in a variety of different contexts. For example, in desktop applications, active leakage power (i.e., leakage power when the processor is computing) is becoming significant compared to switching power. In battery operated systems, standby leakage (i.e., leakage when the processor clock is turned off) dominates as energy is drawn over long idle periods. Increased transistor leakages not only impact the overall power consumed by a CMOS system, but also reduce the margins available for design due to the strong relationship between process variation and leakage power. It is essential for circuit and system designers to understand the components of leakage, sensitivity of leakage to different design parameters, and leakage mitigation techniques in nanometer technologies. This book provides an in-depth treatment of these issues for researchers and product designers. |
No grāmatas satura
6.–10. rezultāts no 67.
5. lappuse
... transistors grew only by about 2.1X every generation, which could be achieved without significant increase in die ... gate tunneling, and junction tunneling leakage components [7,8]. 1.2.1 Gate tunneling leakage With scaling of the ...
... transistors grew only by about 2.1X every generation, which could be achieved without significant increase in die ... gate tunneling, and junction tunneling leakage components [7,8]. 1.2.1 Gate tunneling leakage With scaling of the ...
7. lappuse
... gate depletion effects, both the gate charge and inversion layer charge will be located at a finite distance from ... transistors that promise better transistor aspect ratio [14, 15, 18] are being explored. 1.2.2 Sub-threshold leakage ...
... gate depletion effects, both the gate charge and inversion layer charge will be located at a finite distance from ... transistors that promise better transistor aspect ratio [14, 15, 18] are being explored. 1.2.2 Sub-threshold leakage ...
8. lappuse
... transistors, depends exponentially on its control voltage. In other words the drain current changes exponentially ... Gate voltage Figure 1-6. Relationship between threshold voltage (V) and sub-threshold leakage current (IOFF) for NMOS ...
... transistors, depends exponentially on its control voltage. In other words the drain current changes exponentially ... Gate voltage Figure 1-6. Relationship between threshold voltage (V) and sub-threshold leakage current (IOFF) for NMOS ...
10. lappuse
... gate direct tunneling leakage with oxide thickness scaling limits was mentioned in Section 1.2.1. Scaling of junction depth to maintain the aspect ratio, in scaled transistors, leads to increase in the transistor series resistance ...
... gate direct tunneling leakage with oxide thickness scaling limits was mentioned in Section 1.2.1. Scaling of junction depth to maintain the aspect ratio, in scaled transistors, leads to increase in the transistor series resistance ...
11. lappuse
... gate leakage, while logic transistors will be dominated by sub-threshold leakage. Similarly decoupling capacitors that are used to filter power supply noise are long channel MOS transistors. Therefore these transistors will suffer from ...
... gate leakage, while logic transistors will be dominated by sub-threshold leakage. Similarly decoupling capacitors that are used to filter power supply noise are long channel MOS transistors. Therefore these transistors will suffer from ...
Saturs
Chapter 6 | 141 |
Chapter 7 | 163 |
Chapter 8 | 200 |
L | 209 |
Chapter 9 | 211 |
Chapter 10 | 234 |
VVV0xW+2+ 20 1 | 236 |
Periphery | 254 |
Chapter 4 | 77 |
11 | 81 |
Vdd I t I | 96 |
botas bbarabosse cseldk14keyb long sandsly | 102 |
Chapter 5 | 105 |
6 | 108 |
aget | 121 |
Chapter 11 | 257 |
i | 269 |
i | 274 |
Chapter 12 | 281 |
B | 291 |
Figure 129 Carbon nanotube structures | 298 |
Citi izdevumi - Skatīt visu
Leakage in Nanometer CMOS Technologies Siva G. Narendra,Anantha P. Chandrakasan Ierobežota priekšskatīšana - 2006 |
Leakage in Nanometer CMOS Technologies Siva G. Narendra,Anantha P. Chandrakasan Priekšskatījums nav pieejams - 2005 |
Leakage in Nanometer CMOS Technologies Siva G. Narendra,Anantha P. Chandrakasan Priekšskatījums nav pieejams - 2010 |
Bieži izmantoti vārdi un frāzes
achieved active mode adaptive additional allows applied approach becomes biasing block body bias capacitance cause cell channel length Chapter charge chip circuit clock CMOS compared critical defective delay depends described devices drain drive dynamic effect energy example Figure frequency higher IDDQ IEEE impact implementation improve increase input junction larger leakage current leakage power leakage reduction limit logic lower measured microprocessor minimize MOSFET MTCMOS needed NMOS node noise operation output oxide parameter path penalty performance PMOS power gating power supply power switch presented reduce leakage reduced savings scaling scheme selected shown in Figure shows signal sleep transistor smaller solution speed SRAM stack standby mode sub-threshold leakage substrate supply voltage techniques temperature threshold voltage tunneling turned variation virtual width
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Atsauces uz šo grāmatu
Low Power Methodology Manual: For System-on-Chip Design David Flynn,Rob Aitken,Alan Gibbons,Kaijian Shi Ierobežota priekšskatīšana - 2007 |
Digital Integrated Circuit Design: From VLSI Architectures to CMOS Fabrication Hubert Kaeslin Ierobežota priekšskatīšana - 2008 |